Search results for "quantum field"

showing 10 items of 492 documents

Pion Form Factor Measurement and ISR at BESIII

2017

Abstract At BESIII, we measured the cross section of 900 MeV/c2 with a 2.93 fb−1 data set taken at the center-of-mass energy 3.773 GeV. The initial state radiation technique is used, and the total systematic uncertainty is estimated to be 0.9%. The squared form factor | F π | 2 is extracted, and comparisons are made with results from both KLOE and BaBar. The two-pion contribution to the hadronic vacuum polarization contribution to ( g − 2 ) μ is calculated to be a μ π π , LO ( 600 − 900  MeV / c 2 ) = ( 368.2 ± 2.5 s t a t . ± 3.3 s y s t . ) ⋅ 10 − 10 .

PhysicsSystematic errorNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHadronForm factor (quantum field theory)Radiation01 natural sciencesNuclear physicsPion0103 physical sciencesVacuum polarization010306 general physicsNuclear and Particle Physics Proceedings
researchProduct

Coupled-cluster Theory

2002

PhysicsTheoretical physicsCoupled clusterRelationship between string theory and quantum field theoryAbstract model theory
researchProduct

Electromagnetic Processes and Interactions

2011

The electron, the muon, and their neutrinos are important tools in testing the structure of the fundamental electromagnetic and weak interactions. On the other hand, if these interactions are known, they serve as ideal probes for the internal structure of complex hadronic targets such as nucleons and nuclei. Although electroweak interactions should in fact be discussed as a whole and on the same footing, purely electromagnetic interactions play a distinctive role, for obvious experimental reasons: At low and intermediate energies the effective electromagnetic coupling is larger by many orders of magnitude than the weak couplings, so that electromagnetic processes are measurable to much high…

PhysicsTheoretical physicsMuonOrders of magnitude (time)Electroweak interactionForm factor (quantum field theory)ElectronNeutrinoNucleonDeep inelastic scattering
researchProduct

N-string vertices in string field theory.

1993

We give the general form of the vertex corresponding to the interaction of an arbitrary number of strings. The technique employed relies on the ``comma" representation of String Field Theory where string fields and interactions are represented as matrices and operations between them such as multiplication and trace. The general formulation presented here shows that the interaction vertex of N strings, for any arbitrary N, is given as a function of particular combinations of matrices corresponding to the change of representation between the full string and the half string degrees of freedom.

PhysicsTheoryofComputation_MISCELLANEOUSHigh Energy Physics - TheoryEmpty stringFOS: Physical sciencesFísicaString searching algorithmString field theoryType I string theoryRelationship between string theory and quantum field theoryCombinatoricsNon-critical string theoryHigh Energy Physics::TheoryString operationsHigh Energy Physics - Theory (hep-th)String dualityPhysical review. D, Particles and fields
researchProduct

Topological field theory

1991

PhysicsTopological quantum field theoryTopological algebraTopological degeneracyGeneral Physics and AstronomyTopological orderBF modelTopological entropy in physicsSymmetry protected topological orderGeneral Theoretical PhysicsTopological quantum numberMathematical physicsPhysics Reports
researchProduct

Central region in relativistic heavy ion collisions; results from hydrodynamic calculations and cascade simulation

1988

Results of three dimensional hydrodynamic calculations with boost invariant longitudinal expansion are presented with special emphasis on the transverse momentum spectra of hadrons and production rates of dileptons. The effect and signatures of transverse collective motion are discussed in detail. The hydrodynamic results which are based on the assumption of the existence of a first order phase transition and formation of an equilibrium mixed phase are compared with cascade simulation where the mixed phase is modelled in terms of plasma droplets embedded in a pion gas. The comparison shows a great deal of similarity between the two approaches lending further support for the hydrodynamic app…

PhysicsTransverse planePhase transitionPionCascadeElementary particlePlasmaMechanicsInvariant (physics)Atomic physicsQuantum field theory
researchProduct

Partition Function for the Harmonic Oscillator

2001

We start by making the following changes from Minkowski real time t = x0 to Euclidean “time” τ = tE:

PhysicsVackář oscillatorPartition function (quantum field theory)Vibrational partition functionQuantum harmonic oscillatorQuantum mechanicsAnharmonicityMinkowski spaceMathematics::Metric GeometryParametric oscillatorHarmonic oscillator
researchProduct

Charge Form Factor of the Neutron at Low Momentum Transfer from theH→2(e→,e′n)H1Reaction

2008

We report new measurements of the neutron charge form factor at low momentum transfer using quasielastic electrodisintegration of the deuteron. Longitudinally polarized electrons at an energy of 850 MeV were scattered from an isotopically pure, highly polarized deuterium gas target. The scattered electrons and coincident neutrons were measured by the Bates Large Acceptance Spectrometer Toroid (BLAST) detector. The neutron form factor ratio ${G}_{E}^{n}/{G}_{M}^{n}$ was extracted from the beam-target vector asymmetry ${A}_{\mathrm{ed}}^{V}$ at four-momentum transfers ${Q}^{2}=0.14$, 0.20, 0.29, and $0.42\text{ }\text{ }(\mathrm{GeV}/c{)}^{2}$.

Physicsmedia_common.quotation_subjectNuclear TheoryMomentum transferForm factor (quantum field theory)General Physics and AstronomyCharge (physics)ElectronAsymmetryDeuteriumHigh Energy Physics::ExperimentNeutronAtomic physicsNuclear ExperimentEnergy (signal processing)media_commonPhysical Review Letters
researchProduct

Measuring the Chiralities of Weak b → c(u) Transitions in Exclusive B Meson Decays

1989

I discuss possibilities to measure the chirality of the weak b → c(u) transitions in exclusive bottom meson decays in (i) the exclusive semileptonic decay process B → D* + 1 + ν1 and (ii) in the exclusive nonleptonic decays of bottom mesons to baryon-antibaryon pairs.

Physics::Fluid DynamicsSemileptonic decayChiralityPhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::PhenomenologyForm factor (quantum field theory)High Energy Physics::ExperimentB mesonNuclear Experiment
researchProduct

New physics vs new paradigms: distinguishing CPT violation from NSI

2019

Our way of describing Nature is based on local relativistic quantum field theories, and then CPT symmetry, a natural consequence of Lorentz invariance, locality and hermiticity of the Hamiltonian, is one of the few if not the only prediction that all of them share. Therefore, testing CPT invariance does not test a particular model but the whole paradigm. Current and future long baseline experiments will assess the status of CPT in the neutrino sector at an unprecedented level and thus its distinction from similar experimental signatures arising from non-standard interactions is imperative. Whether the whole paradigm is at stake or just the standard model of neutrinos crucially depends on th…

Physics::General PhysicsPhysics and Astronomy (miscellaneous)CPT symmetryPhysics beyond the Standard ModelFOS: Physical scienceslcsh:AstrophysicsLorentz covariance01 natural sciencesPartícules (Física nuclear)High Energy Physics - Experimentsymbols.namesakeTheoretical physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuantum field theory010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsLocalityHigh Energy Physics::PhenomenologyHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentNeutrinoHamiltonian (quantum mechanics)
researchProduct